The moment of inertia of a solid disc about its central axis (perpendicular to its plane) is: \[ I = \frac{1}{2}MR^2 \]
For the first disc: \[ I_1 = \frac{1}{2} M_1 R_1^2 \] For the second disc: \[ I_2 = \frac{1}{2} M_2 R_2^2 \]
It is given that: \[ R_2 = 2R_1 \]
Since the discs are made of iron (same material), the mass is proportional to the area (assuming thickness is negligible). So: \[ \frac{M_2}{M_1} = \left( \frac{R_2}{R_1} \right)^2 = \left( \frac{2R_1}{R_1} \right)^2 = 4 \] \[ M_2 = 4M_1 \]
Substituting the values: \[ I_1 = \frac{1}{2} M_1 R_1^2 \] \[ I_2 = \frac{1}{2} \times 4M_1 \times (2R_1)^2 = \frac{1}{2} \times 4M_1 \times 4R_1^2 = 8M_1R_1^2 \]
Ratio \( \frac{I_1}{I_2} \): \[ \frac{I_1}{I_2} = \frac{\frac{1}{2} M_1 R_1^2}{8M_1R_1^2} = \frac{1}{2 \times 8} = \frac{1}{16} \]
Therefore, \[ \boldsymbol{x = 16} \]
A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.